    i (0.66 0.03stat 0.02sys)]    GeV2 ,

where the first error is statistical and the second systematic. This final
value, which is indicated in gray in Fig. REF  (with the
errors added in quadrature), is in agreement with other results available
in the literature [1]}, [2]}, [3]}, [4]}. Thus, the Padés clearly favor a pair of complex
poles, with an imaginary part inconsistent with zero,
for the Landau-gauge gluon propagator.
<FIGURE>